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Table 1.

MIR emission line fluxes from MIRI/MRS channels, in units of MegaJansky/steradians.

Line Wave Channel I.P. N Flux
[μm] [eV] [106 MJy/sr]

H2S(1) 17.035 3C 1 14.4 ± 0.3
H2S(2) 12.279 3A 1 1.96 ± 0.06
H2S(3) 9.665 2B 1 2.42 ± 0.08
H2S(4) 8.026 2A 1 0.46 ± 0.01
H2S(5) 6.909 1C 1 1.19 ± 0.02
[SIV] 10.511 2C 34.79 2 22.6 ± 0.4
[SIII] 18.713 4A 23.34 2 7.7 ± 0.2
[ArII] 6.985 1C 15.76 2 4.9 ± 0.7
[ArIII] 8.991 2B 27.63 2 4.10 ± 0.07
[ArV] 13.102 2B 59.81 1 0.501 ± 0.008
[MgV] 5.609 1A 109.24 2 2.64 ± 0.04
[MgVII] 5.503 1A 186.51 2 1.33 ± 0.02
[NeVI] 7.652 2A 126.21 2 8.6 ± 0.1
[NeII] 12.814 3A 21.56 2 23.0 ± 0.4
[NeV] 14.322 3B 97.12 2 42.0 ± 0.6
[NeIII] 15.555 3C 40.96 2 64 ± 1
[NeV] 24.318 4B 97.12 2 14.4 ± 0.4
[OIV] 25.890 4C 54.93 2 74 ± 2
FeII 5.340 1A 7.90 2 1.50 ± 0.03
FeVIII 5.447 1A 124.80 2 24.2 ± 0.3
FeVII 9.527 2B 99.10 2 1.57 ± 0.02

Notes. From left to right: Line name, rest-frame wavelength, MIRI/MRS sub-channel, ionisation potential of the transition, maximum number of Gaussian components used to fit the line profile. Fluxes were obtained by integrating the best-fit multi-Gaussian model of the reduced data cubes considering spaxels at S/N ≥ 2 within the FoV of Channel 1, which is in common to all channels, without subtracting the PSF.

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